Classical Electrodynamics |
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Page 286
This is analogous to the geometrical situation shown in the left side of Fig. 9.5.
We do not care about the values of the fields in region II". In fact, the hypothetical
sources inside the disc will be imagined to be such that the fields in region II' give
...
This is analogous to the geometrical situation shown in the left side of Fig. 9.5.
We do not care about the values of the fields in region II". In fact, the hypothetical
sources inside the disc will be imagined to be such that the fields in region II' give
...
Page 392
:For,. (12.1) where v, * (v,ic), and F., is interpreted as the average field acting on
the particle. The left-hand side of (12.1) is now to be equated to the time rate of
change of the momentum and energy of the particle, just as in ...
:For,. (12.1) where v, * (v,ic), and F., is interpreted as the average field acting on
the particle. The left-hand side of (12.1) is now to be equated to the time rate of
change of the momentum and energy of the particle, just as in ...
Page 417
On the left-hand side of the figure is a constant, uniform magnetic induction Bo,
parallel to the c axis. ... We wish to treat that motion as a zero-order
approximation to the motion of the particle in the field shown on the righthand
side of the figure, ...
On the left-hand side of the figure is a constant, uniform magnetic induction Bo,
parallel to the c axis. ... We wish to treat that motion as a zero-order
approximation to the motion of the particle in the field shown on the righthand
side of the figure, ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
BoundaryValue Problems in Electrostatics II | 54 |
Copyright | |
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